Jump to
S1C2
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -375.670900 |
| Energy at 298.15K | |
| HF Energy | -375.670900 |
| Nuclear repulsion energy | 189.345351 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3390 |
3061 |
22.48 |
41.08 |
0.11 |
0.19 |
| 2 |
A |
3368 |
3041 |
4.33 |
80.42 |
0.64 |
0.78 |
| 3 |
A |
3299 |
2978 |
7.37 |
98.02 |
0.10 |
0.18 |
| 4 |
A |
1670 |
1508 |
5.41 |
9.41 |
0.75 |
0.86 |
| 5 |
A |
1596 |
1441 |
10.31 |
2.41 |
0.72 |
0.84 |
| 6 |
A |
1545 |
1395 |
28.16 |
5.66 |
0.75 |
0.86 |
| 7 |
A |
1476 |
1333 |
21.84 |
2.89 |
0.74 |
0.85 |
| 8 |
A |
1368 |
1235 |
15.46 |
10.39 |
0.72 |
0.84 |
| 9 |
A |
1261 |
1139 |
56.14 |
7.85 |
0.74 |
0.85 |
| 10 |
A |
1237 |
1117 |
59.57 |
4.26 |
0.61 |
0.76 |
| 11 |
A |
1183 |
1068 |
166.09 |
3.21 |
0.37 |
0.54 |
| 12 |
A |
1136 |
1025 |
61.15 |
8.94 |
0.46 |
0.63 |
| 13 |
A |
997 |
900 |
48.82 |
7.28 |
0.28 |
0.44 |
| 14 |
A |
592 |
534 |
9.58 |
2.56 |
0.34 |
0.51 |
| 15 |
A |
503 |
454 |
35.32 |
0.94 |
0.73 |
0.85 |
| 16 |
A |
442 |
399 |
11.16 |
2.05 |
0.54 |
0.70 |
| 17 |
A |
262 |
236 |
17.28 |
0.09 |
0.58 |
0.73 |
| 18 |
A |
121 |
109 |
16.68 |
0.05 |
0.71 |
0.83 |
Unscaled Zero Point Vibrational Energy (zpe) 12722.1 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 11486.8 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/6-31G
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.758 |
-0.581 |
-0.322 |
| C2 |
0.448 |
0.018 |
0.332 |
| F3 |
-1.892 |
0.095 |
0.173 |
| F4 |
1.539 |
-0.778 |
0.010 |
| F5 |
0.692 |
1.277 |
-0.183 |
| H6 |
-0.719 |
-0.451 |
-1.389 |
| H7 |
-0.849 |
-1.622 |
-0.066 |
| H8 |
0.380 |
0.098 |
1.398 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.4976 | 1.4097 | 2.3293 | 2.3620 | 1.0756 | 1.0756 | 2.1721 |
C2 | 1.4976 | | 2.3466 | 1.3881 | 1.3822 | 2.1313 | 2.1283 | 1.0716 | F3 | 1.4097 | 2.3466 | | 3.5436 | 2.8641 | 2.0281 | 2.0234 | 2.5816 | F4 | 2.3293 | 1.3881 | 3.5436 | | 2.2311 | 2.6758 | 2.5331 | 2.0093 | F5 | 2.3620 | 1.3822 | 2.8641 | 2.2311 | | 2.5359 | 3.2856 | 1.9973 | H6 | 1.0756 | 2.1313 | 2.0281 | 2.6758 | 2.5359 | | 1.7721 | 3.0460 | H7 | 1.0756 | 2.1283 | 2.0234 | 2.5331 | 3.2856 | 1.7721 | | 2.5716 | H8 | 2.1721 | 1.0716 | 2.5816 | 2.0093 | 1.9973 | 3.0460 | 2.5716 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
107.581 |
|
C1 |
C2 |
F5 |
110.143 |
| C1 |
C2 |
H8 |
114.426 |
|
C2 |
C1 |
F3 |
107.601 |
| C2 |
C1 |
H6 |
110.777 |
|
C2 |
C1 |
H7 |
110.534 |
| F3 |
C1 |
H6 |
108.633 |
|
F3 |
C1 |
H7 |
108.259 |
| F4 |
C2 |
F5 |
107.286 |
|
F4 |
C2 |
H8 |
108.867 |
| F5 |
C2 |
H8 |
108.302 |
|
H6 |
C1 |
H7 |
110.924 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.063 |
|
|
|
| 2 |
C |
0.615 |
|
|
|
| 3 |
F |
-0.444 |
|
|
|
| 4 |
F |
-0.433 |
|
|
|
| 5 |
F |
-0.421 |
|
|
|
| 6 |
H |
0.214 |
|
|
|
| 7 |
H |
0.199 |
|
|
|
| 8 |
H |
0.208 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.416 |
-2.036 |
0.430 |
2.122 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.210 |
2.231 |
2.153 |
| y |
2.231 |
-28.716 |
0.865 |
| z |
2.153 |
0.865 |
-24.050 |
|
| Traceless |
| | x | y | z |
| x |
-8.827 |
2.231 |
2.153 |
| y |
2.231 |
0.914 |
0.865 |
| z |
2.153 |
0.865 |
7.913 |
|
| Polar |
| 3z2-r2 | 15.826 |
| x2-y2 | -6.494 |
| xy | 2.231 |
| xz | 2.153 |
| yz | 0.865 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.956 |
-0.140 |
-0.087 |
| y |
-0.140 |
3.049 |
0.004 |
| z |
-0.087 |
0.004 |
2.810 |
<r2> (average value of r
2) Å
2
| <r2> |
113.019 |
| (<r2>)1/2 |
10.631 |
Jump to
S1C1
Energy calculated at HF/6-31G
| | hartrees |
| Energy at 0K | -375.666150 |
| Energy at 298.15K | |
| HF Energy | -375.666150 |
| Nuclear repulsion energy | 192.380430 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HF/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3348 |
3023 |
30.00 |
81.91 |
0.18 |
0.30 |
| 2 |
A' |
3285 |
2966 |
8.48 |
90.06 |
0.15 |
0.26 |
| 3 |
A' |
1667 |
1505 |
5.00 |
9.30 |
0.75 |
0.86 |
| 4 |
A' |
1580 |
1426 |
9.13 |
0.58 |
0.69 |
0.82 |
| 5 |
A' |
1556 |
1405 |
31.58 |
5.36 |
0.70 |
0.82 |
| 6 |
A' |
1276 |
1152 |
101.39 |
8.36 |
0.52 |
0.68 |
| 7 |
A' |
1151 |
1039 |
11.96 |
4.90 |
0.75 |
0.86 |
| 8 |
A' |
952 |
860 |
62.13 |
10.34 |
0.08 |
0.14 |
| 9 |
A' |
790 |
713 |
74.34 |
3.87 |
0.57 |
0.72 |
| 10 |
A' |
512 |
462 |
24.66 |
2.05 |
0.75 |
0.86 |
| 11 |
A' |
249 |
225 |
3.60 |
0.22 |
0.55 |
0.71 |
| 12 |
A" |
3351 |
3026 |
12.92 |
51.56 |
0.75 |
0.86 |
| 13 |
A" |
1540 |
1391 |
36.16 |
1.86 |
0.75 |
0.86 |
| 14 |
A" |
1391 |
1256 |
19.55 |
19.74 |
0.75 |
0.86 |
| 15 |
A" |
1245 |
1124 |
78.20 |
1.58 |
0.75 |
0.86 |
| 16 |
A" |
1061 |
958 |
74.55 |
5.66 |
0.75 |
0.86 |
| 17 |
A" |
392 |
354 |
0.15 |
0.29 |
0.75 |
0.86 |
| 18 |
A" |
121 |
109 |
4.52 |
0.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12733.6 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 11497.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HF/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.761 |
-0.816 |
0.000 |
| C2 |
0.369 |
0.627 |
0.000 |
| F3 |
-0.394 |
-1.615 |
0.000 |
| F4 |
-0.394 |
0.915 |
1.116 |
| F5 |
-0.394 |
0.915 |
-1.116 |
| H6 |
1.328 |
-1.048 |
-0.885 |
| H7 |
1.328 |
-1.048 |
0.885 |
| H8 |
1.217 |
1.286 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
F3 |
F4 |
F5 |
H6 |
H7 |
H8 |
| C1 | | 1.4954 | 1.4044 | 2.3619 | 2.3619 | 1.0767 | 1.0767 | 2.1512 |
C2 | 1.4954 | | 2.3680 | 1.3827 | 1.3827 | 2.1236 | 2.1236 | 1.0742 | F3 | 1.4044 | 2.3680 | | 2.7655 | 2.7655 | 2.0179 | 2.0179 | 3.3183 | F4 | 2.3619 | 1.3827 | 2.7655 | | 2.2330 | 3.2906 | 2.6220 | 1.9949 | F5 | 2.3619 | 1.3827 | 2.7655 | 2.2330 | | 2.6220 | 3.2906 | 1.9949 | H6 | 1.0767 | 2.1236 | 2.0179 | 3.2906 | 2.6220 | | 1.7704 | 2.4989 | H7 | 1.0767 | 2.1236 | 2.0179 | 2.6220 | 3.2906 | 1.7704 | | 2.4989 | H8 | 2.1512 | 1.0742 | 3.3183 | 1.9949 | 1.9949 | 2.4989 | 2.4989 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
F4 |
110.239 |
|
C1 |
C2 |
F5 |
110.239 |
| C1 |
C2 |
H8 |
112.656 |
|
C2 |
C1 |
F3 |
109.456 |
| C2 |
C1 |
H6 |
110.246 |
|
C2 |
C1 |
H7 |
110.246 |
| F3 |
C1 |
H6 |
108.116 |
|
F3 |
C1 |
H7 |
108.116 |
| F4 |
C2 |
F5 |
107.705 |
|
F4 |
C2 |
H8 |
107.918 |
| F5 |
C2 |
H8 |
107.918 |
|
H6 |
C1 |
H7 |
110.602 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.076 |
|
|
|
| 2 |
C |
0.620 |
|
|
|
| 3 |
F |
-0.431 |
|
|
|
| 4 |
F |
-0.420 |
|
|
|
| 5 |
F |
-0.420 |
|
|
|
| 6 |
H |
0.195 |
|
|
|
| 7 |
H |
0.195 |
|
|
|
| 8 |
H |
0.186 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
4.597 |
0.201 |
0.000 |
4.601 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.759 |
-0.440 |
0.000 |
| y |
-0.440 |
-29.755 |
0.000 |
| z |
0.000 |
0.000 |
-29.748 |
|
| Traceless |
| | x | y | z |
| x |
4.992 |
-0.440 |
0.000 |
| y |
-0.440 |
-2.502 |
0.000 |
| z |
0.000 |
0.000 |
-2.491 |
|
| Polar |
| 3z2-r2 | -4.981 |
| x2-y2 | 4.996 |
| xy | -0.440 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.988 |
0.074 |
0.000 |
| y |
0.074 |
2.836 |
0.000 |
| z |
0.000 |
0.000 |
3.073 |
<r2> (average value of r
2) Å
2
| <r2> |
103.795 |
| (<r2>)1/2 |
10.188 |